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(11) | EP 0 959 479 B1 |
| (12) | EUROPEAN PATENT SPECIFICATION |
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A method for controlling velocity of an armature of an electromagnetic actuator Verfahren zur Regelung der Geschwindigkeit eines Ankers in einem elektromagnetischem Aktuator Procédé de régulation pour la vitesse de l'armature d'un actionneur électromagnétique |
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| Note: Within nine months from the publication of the mention of the grant of the European patent, any person may give notice to the European Patent Office of opposition to the European patent granted. Notice of opposition shall be filed in a written reasoned statement. It shall not be deemed to have been filed until the opposition fee has been paid. (Art. 99(1) European Patent Convention). |
[0001] This application claims the benefit of U.S. Provisional Application No. 60/083,351, filed April 28, 1998, and U.S. Provisional Application No. 60/083,329, filed April 28, 1998.
BACKGROUND OF THE INVENTION
1. Field of the invention
[0002] This invention relates to a high-speed, high-force electromagnetic actuator and more particularly, to an electromagnetic actuator for opening and closing a valve of an internal combustion engine wherein a velocity of the armature is controlled upon landing against a stator core of the actuator.
2. Description of Related Art
[0003] A conventional electromagnetic actuator for opening and closing a valve of an internal combustion engine generally includes an electromagnet which, when energized, produces an electromagnetic force on an armature. The armature is biased by a return spring and the armature is coupled with a cylinder valve of the engine. The armature is held by the electromagnet in one operating position against a stator core of the actuator and, by deenergizing the electromagnet, the armature may move towards and into another operating position by the return spring.
[0004] In an attempt to control the landing velocity of the armature, in certain electromagnetic actuator systems, power to a coil of the actuator is applied to move the armature across a gap and when the armature is approaching the stator core, a magnetic force from the coil is removed to slow down the armature and hope for a quiet or "soft" (near zero velocity) landing. Just before landing, the stator coil is reenergized to draw the armature towards and land at the stator core.
[0005] In this type of arrangement, landing of the armature at a stator core is quite harsh and may have a velocity of approximately one meter per second. However, a required velocity value of the armature at landing calculated to provide acceptably quiet actuator operation is less than 0.04 meters per second at 600 engine rpm and less than 0.4 meters per second 6,000 engine rpm.
[0006] Accordingly, there is a need to provide control of an armature of an electromagnetic actuator to ensure that the armature completes its travel during its stroke but at the same time produces a quiet or "soft" (near zero velocity) landing of the armature against a stator core so as to prevent excessive impact wear on the armature and stator core and to reduce the amount of noise produced by such impact.
[0007] US-A-5708355 describes a method of controlling an electromagnetic actuator having at least one electromagnet and an armature that can be moved against a restoring spring. An actual time of impact is derived and if it is earlier or later than an expected time of impact, then the switch on time for the capturing electromagnet is changed in a subsequent cycle to improve the chances of the time of impact being correct the next time.
[0008] Also document DE 1 9544207 shows an electromagnetic actuator and a method to control the armature landing speed.
SUMMARY OF THE INVENTION
[0009] In accordance with a first aspect of the present invention a method of controlling velocity of an armature of an electromagnetic actuator as the armature moves from a first position towards a second position, the electromagnetic actuator including a coil and a core at said second position, said coil generating a magnetic force to cause the armature to move towards and land at said core, and spring structure acting on the armature to bias the armature away from said second position to a resetting position, the method comprising selectively energizing said coil to permit said armature to move at a certain velocity towards said core; the method further comprising determining a certain voltage corresponding to a voltage across said coil when said armature is moving toward said core; and using said certain voltage as a feedback variable to control energy to said coil so as to control a velocity of said armature as said armature moves towards said core; characterised in that the step of determining said certain voltage includes providing a parametrically determined voltage which mirrors a terminal voltage of said coil, said parametrically determined voltage defining said certain voltage.
[0010] In accordance with a second aspect of the present invention, an electromagnetic actuator comprises an armature movable between first and second positions during a stroke of a cycle;
spring structure biasing said armature towards a resetting position generally between said first and second positions;
a stator having a coil and a core at said first position, said coil being constructed and arranged to apply a magnetic force, when energized, to the armature to cause the armature to move towards and land at said core and to maintain said armature at said core for a predetermined period;
circuit structure providing a certain voltage which corresponds to magnetic flux of a magnetic circuit created by said coil, core and said armature; and
control structure to control movement of said armature, wherein said control structure is constructed and arranged to determine said certain voltage when said armature is approaching said core, and to use said certain voltage as a feedback variable to control energy to said coil and thus control a velocity of said armature as said armature moves towards said core; characterised in that said circuit structure is constructed and arranged to provide a parametrically determined voltage which mirrors a terminal voltage of said coil, said control structure using said parametrically determined voltage as said feedback variable, said parametrically determined voltage defining said certain voltage.
[0011] An object of the present invention is to fulfill the need referred to above. In accordance with the principles of the present invention, this objective is obtained by providing a method of controlling velocity of an armature of an electromagnetic actuator as the armature moves from a first position towards a second position. The electromagnetic actuator includes a coil and a core at the second position. The coil generates a magnetic force to cause the armature to move towards and land at the core. Spring structure acts on the armature to bias the armature away from the second position to a resetting position. The method includes selectively energizing the coil to permit the armature to move at a certain velocity towards the core. A certain voltage corresponding to a voltage across the coil is determined when the armature is approaching the core. The certain voltage is used as a feedback variable to control energy to the coil so as to control a velocity of the armature as the armature moves towards the core. In one embodiment, the certain voltage is a measured terminal voltage of the coil. In another embodiment, the certain voltage is a parametrically determined voltage which mirrors the coil terminal voltage.
[0012] In accordance with another aspect of the invention, an electromagnetic actuator is provided and includes an armature movable between first and second positions. Spring structure biases the armature towards a resetting position generally between the first and second positions. A stator is provided which has a coil and a core at the first position. The coil, when energized, applies a magnetic force to the armature to cause the armature to move towards and land at the core and to maintain the armature at the core for a predetermined period. Circuit structure provides a certain voltage which corresponds to a rate of change of magnetic flux of a magnetic circuit created by the coil and the armature. Control structure controls movement of the armature. The control structure is constructed and arranged to determine the certain voltage when the armature is approaching the core, and to use the certain voltage as a feedback variable to control the rate of change of magnetic flux and thus control a velocity of the armature as the armature moves towards the core.
[0013] Other objects, features and characteristics of the present invention, as well as the methods of operation and the functions of the related elements of the structure, the combination of parts and economics of manufacture will become more apparent upon consideration of the following detailed description and appended claims with reference to the accompanying drawings,'all of which form a part of this specification.
BRIEF DESCRIPTION OF THE DRAWING
[0014]
FIG. 1 is a sectional view of an electromagnetic actuator provided in accordance with the principles of the present invention, shown in a valve open position;
FIG. 2 is a sectional view of the electromagnetic actuator of FIG. 1, but shown in a valve closed position;
FIG. 3 is a waveform as applied to an electromagnetic actuator of the invention operating in an open loop control mode;
FIG. 4 is a waveform of flux generation of an electromagnetic actuator of the invention in an open loop mode of operation;
FIG. 5 is a schematic representation of a solenoid coil of the electromagnetic actuator of FIG. 1, shown connected electrically to a programable current regulator,
FIG. 6 are waveforms of an actuator of the invention showing coil terminal voltage, an integral of the terminal voltage, measured magnetic flux and the derivative of the measured magnetic flux, to illustrate the relationships between terminal voltage and magnetic flux;
FIG. 7 is a block diagram of a control circuit for the electromagnetic actuator in accordance with a first embodiment of the present invention;
FIG. 8 is a graphical representation of an actuator of the invention operating in a closed loop mode and when approaching a landing position, showing a current waveform, a voltage waveform, a position waveform and a flux waveform;
FIG. 9 is a block diagram of a mirror circuit for an electromagnetic actuator provided in accordance with a second embodiment of the invention; and
FIG. 10 are waveforms of an electromagnetic actuator of the invention operating in a closed loop mode, utilizing the circuit of FIG. 9, to provide a soft landing of the armature of the actuator.
DETAILED DESCRIPTION OF THE INVENTION
[0015] Referring to FIGS. 1 and 2, an electromagnetic actuator is shown, generally indicated 10, provided in accordance with the principles of the present invention. The electromagnetic actuator 10 includes a first electromagnet, generally indicated at 12, which includes a stator core 14 and a solenoid coil 16 associated with the stator core 14. A second electromagnet, generally indicated at 18, is disposed generally in opposing relation to the first electromagnet 12. The second electromagnet includes a stator core 20 and a solenoid coil 22 associated with the stator core 20. The electromagnetic actuator 10 includes an armature 24 which is attached to a stem 26 of a cylinder valve 28 through a hydraulic valve adjuster 27. The armature 24 is disposed generally between the electromagnets 12 and 18 so as to be acted upon by the electromagnetic force created by the electromagnets. In a deenergized state of the electromagnets 12 and 18, the armature 24 is maintained in a position of rest (a resetting position) generally between the two electromagnets 12 and 18 by opposing working return springs 30 and 32. In a valve close position (FIG 2), the armature 24 engages the stator core 14 of the first electromagnet 12.
[0016] To initiate motion of the armature 24 and thus the valve 28 from the closed position into an open position (FIG. 1), a holding current through solenoid coil 16 of the first electromagnet 12 is discontinued. As a result, a holding force of the electromagnet 12 falls below the spring force of the return spring 30 and thus the armature 24 begins its motion accelerated by the return spring 30. To catch the armature 24 in the open position, a catch current is applied to the electromagnet 18. Once the armature has landed at the stator core 20, the catch current is changed to a hold current which is sufficient to hold the armature at the stator core 20 for a predetermined period of time.
[0017] FIG. 3 shows a system voltage timing waveform 31 of coil 16 of the electromagnetic actuator 10 in an open loop mode of operation. To initiate movement of the armature and thus move the valve 28 from a valve open position shown in FIG. 1 to a valve closed position as shown a FIG. 2, full voltage is applied to the first solenoid coil 16 at the beginning of armature stroke at time T0. Simultaneously, power is removed from the second solenoid coil 22 to release the armature 24 from the second stator core 20. Once the armature 24 is moving, voltage at the solenoid coil 16 is removed at the time T1 to permit the armature 24 to travel as a spring mass system under simple harmonic motion until it is near closing. At time T2, full coil voltage is applied to the coil 16 to initiate a catch current phase. Finally, at a time T3, the coil voltage on the receiving coil 16 is reduced to a value sufficient to hold the armature 24 to the stator core 14 against the bias of return spring 30.
[0018] FIG. 4 is a simplified flux waveform 33 of the electromagnetic actuator 10 in an open loop mode of operation as obtained by a Hall sensor. When an initial voltage pulse is applied to a solenoid coil, e.g., coil 16, flux begins to build up until T1. At time T1, the voltage is removed and as the armature 24 is moving across the gap 32, there is only a slight amount flux increase. At time T2, the voltage is re-applied to the coil 16, the flux increases rapidly and at time T3 the voltage is reduced to provide a holding current. In theory, values can be calculated for time T1, T2 and T3 to achieve a desirable soft landing of the armature 24 against a stator core. In practice, however, this is almost never achievable because the system is constantly being perturbed by real world variation parameters such as damping, temperature, deflections, tolerance stack up, vibration, engine gas loads, etc.
[0019] From the above discussion, is clear that some form of feedback algorithm is required to increase the robustness of the armature control to ensure a soft landing thereof.
[0020] U. S. Patent Application No. 09/025,986, entitled "Electronically Controlling the Landing of an Armature in an Electromagnetic Actuator", discloses using a flux sensor to sense a rate of change of magnetic flux in an electromagnetic actuator. The rate of change of flux sensed is used as a feedback variable to control a landing velocity of an armature of the actuator by controlling the catch current. Sensing flux for feedback control of an electromagnetic actuator has two distinct advantages over other available parameters: (1) it is extremely sensitive in response (inverse square law) to armature motion in a region near landing of the armature, and (2) its signal voltage is monotonically increasing with increasing displacement of the armature. These features do not apply to parameters such as position, velocity, or electrical current. The use of a flux sensor in an electromagnetic actuator is effective in operation, however, the cost of the actuator is increased due to the need for one or more flux sensors.
[0021] The invention provides feedback control based on a rate of change of flux without the need for a flux sensor. Thus, in accordance with one aspect of the invention, coil 16 (FIG. 5) is connected electrically to a programable current regulator 34. Description of operation is made with regard to coil 16 and core 14 of the first electromagnet. It can be appreciated that this description applies to the operation of the second electromagnet as well. As is commonly employed, a current level of a sufficiently large value is initially commanded in the solenoid coil 16 to achieve rapid movement of the armature 24 through its stroke. The current level is then reduced to a value just enough to hold the armature 24 in contact with the associated stator core 14 until the end of a desired cycle for the actuator 10 at which time current is reduced zero. As shown in FIG. 5, the solenoid coil 16 has been represented as a pure inductance in series with its internal resistance 36 and the current regulator 34 is a "black box equivalent". The resistance R is essentially constant during this analysis but the inductance L(t) is seen to be time varying as a function of (primarily) the position of the armature and (secondarily) the magnetic hysteresis properties with respect to magnetomotive force induced in the ferrous material of the armature 24 and associated stator core 14.
[0022] Applying Kirchoff's Voltage Law around this simple series circuit shows that the terminal voltage from (a) to (b) of the current regulator must at all times equal the sum of the IR drop on the internal resistance R and the counter electromotive force (EMF) of the coil. This is expressed mathematically in the following equation:
[0023] Furthermore, by Faraday's Law, the EMF of a coil having N number of turns equals the product of the number of turns times the rate of change of flux in the coil 16. In applications such as a solenoid coil for an electromagnetic actuator for a valve of an internal combustion engine, the coil EMF is quite large during activation of the armature (100 volts typical) while the IR drop term in Equation 1 is small enough to be negligible for the purpose of sensing the rate of change of flux (6 to 8 volts typical). Therefore, the terminal voltage on the coil 16 is nearly in exact proportion to the time rate of change of the flux in the actuator 10 during operation. Thus, this terminal voltage can be utilized as a feedback variable to control soft landing of the armature 24 of the electromagnetic actuator 10, without the need for any external flux sensor.
[0024] FIG. 6 shows waveforms of an actuator of the invention including a terminal voltage of a coil of the actuator, an integral of the terminal voltage, magnetic flux as obtained by a flux sensor for comparative purposes, and the derivative of the magnetic flux. The applicants have determined a relationship exists between the terminal voltage and the derivative of magnetic flux. This relationship is clearly shown in FIG. 6. In addition, the integral of the terminal voltage is seen to be proportional to the level of magnetic flux in the armature-stator magnetic circuit.
[0025] With reference to FIG. 7, a block diagram of an operating circuit according to one embodiment of the present invention is shown. The circuit is based on controlling the armature velocity near landing by regulating a rate of change of magnetic flux in the armature/stator magnetic circuit by measuring the terminal voltage of the coil. In the circuit of the FIG. 7, a terminal voltage 36 of a coil 16 is applied to a comparator 38. A threshold level 40 is also applied to the comparator 38. The output of the comparator 38 is "logically added" with a logic timing component 42 and is supplied to a drive circuit 44 to drive an actuator 10. Once the actuator driver is energized, the solenoid coil 16 is energized.
[0026] The measured coil terminal voltage 36, corresponding to the rate of change of magnetic flux, is compared to the threshold level 40. The threshold level 40 is set at a desired rate of change of magnetic flux at certain operating conditions of the actuator to produce a soft landing of the armature. If the terminal voltage 36 is above the threshold level 40, the catch current supplied to the solenoid coil 16 is decreased, and if the terminal voltage 36 is below the threshold level 40, the catch current supplied to the solenoid coil 16 is increased, thus controlling the magnetic flux 41 between T2 and T3 as indicated in FIG. 8. This is a closed loop control and the velocity waveform labeled "V" in FIG. 8 illustrates the landing velocity near zero at or near T3. The magnetic flux waveform obtained from a flux sensor is indicated at "F" in FIG. 8 for comparative purposes. The current waveform of a coil is indicated at "I" in FIG. 8. The dip 46 in the current when the armature 24 seats at a stator core is illustrated. Finally, the wave shape labeled "A" in FIG. 8 indicates the movement of the armature 24 from an initial position to a landing position at a stator core.
[0027] It is noted that the flux buildup is generally linear near impact of the armature 24 with a stator core, e.g., core 14. The buildup of the flux in this region 45 between T2 and T3 is controlled by controlling the catch current and defines an inclined line. Thus, as the armature 24 is approaching landing, the flux is inhibited, modulating the magnetic force from the receiving stator core 14 and coil 16 and causing the velocity of the armature 24 to approach zero. At T3, the flux is no longer inhibited and the armature 24 is held against the stator core 14.
[0028] The final value of flux, which is the force on the armature, is set at T3 to the hold current so as to just exceed the opposing spring force created by spring 30. This permits rapid release of the armature 24 at the beginning of the next stroke of the valve 28. In addition, the hold current minimizes the power required to control the actuator 10.
[0029] Although measuring the coil terminal voltage directly is effective for controlling soft landing of the armature 24 of an actuator 10, it is preferable to not physically measure the high common mode voltage typically present at each terminal of the coil. In an electromagnetic actuator 10 of the type used to control valves of an internal combustion engine, the required common mode rejection ratio (CMRR) for the sensing amplifier is on the order of 60 db. While this CMRR is within the state-of-the-art for integrated circuit amplifiers, the real world applications of such measurement suffer from offset drift and electrical interference due to extremely high dV/dt at the voltage being measured.
[0030] Thus, in accordance with the principles of the present invention, a mirror image of the coil terminal voltage and hence a mirror image of the rate of change of flux in the actuator's magnetic circuit is provided by the circuit of the actuator 10 such that there is no need to physically monitor the coil terminals to measure the coil terminal voltage.
[0031] FIG. 9 shows a block diagram of a mirror circuit 43 the actuator 10 provided in accordance with the principles of the present invention. The solenoid coil 16 of the actuator 10 is driven preferably by a pulse width modulation (PWM) (switchmode) current regulator 50 which provides a pulse train to a high voltage power transistor stage (including a high operating voltage supply 52 and a power switch 54) which subsequently switches voltage pulses across the load of the coil 16. It can be appreciated that power can be regulated by other means, such as, for example, a voltage regulator or amplifier. The flux mirror addition to this conventional approach consists of routing the logic level PWM signal from the current regulator 50 through a buffer 56. The rail voltage of the buffer 56 is derived from a scaled-down replica of the system high voltage supply 52. Finally, the scaled and buffered pulse train 58 is smoothed by a low pass filter 60.
[0032] The time constant of the low pass filter 60 is selected to match the rate of armature motion in the actuator 10. The output from the low pass filter 60 is scaled-down from and mirroring the high operating voltage of the coil and corresponds to the desired time rate of change of magnetic flux d(phi)/dt which is used as a feedback variable to control the landing velocity of the armature 24 in the manner discussed above.
[0033] The mirror circuit of the invention is much less troublesome to implement in real world applications due to the reduction or elimination of problems caused by both CMRR requirements and interference from high dV/dt.
[0034] FIG. 10 shows waveforms of an electromagnetic actuator 10 being controlled by the mirror circuit of FIG. 8. "V" is the armature velocity which, as shown, decreases to zero near T3. The coil current is indicated at "I" and the dip 46 in the current occurs at T3. The actual magnetic flux is indicated at "F" which was obtained by a flux sensor and is illustrated for comparative purposes. The rate of change of magnetic flux d(phi)/dt is shown which corresponds to a parametrically determined voltage obtained from the mirror circuit of FIG. 9. The applicants have found that the rate of change of magnetic flux d(phi)/dt is controlled to be generally constant between T2 and T3 which is found to be optimal for providing the desired soft landing of the armature 24 at a stator core. By controlling the rate of change of magnetic flux between T2 and T3 in this manner, the highly non-linear characteristic of the flux buildup (and hence the force on the armature) is eliminated to provide the desired soft landing of the armature.
[0035] It has thus been seen that the objects of this invention have been fully and effectively accomplished. It will be realized, however, that the foregoing preferred embodiments have been shown and described for the purposes of illustrating the structural and functional principles of the present invention, as well as illustrating the methods of employing the preferred embodiments and are subject to change without departing from such principles.
routing a logic level signal from the current regulator through said buffer, rail voltage at said buffer being derived from a scaled-down replica of a high voltage supply of said actuator, and
smoothing a scaled and buffered pulse train from said buffer with said low pass filter, an output of said low pass filter defining said parametrically determined voltage.
selectively energizing the other of said coils to draw said armature at a certain velocity towards the core associated with said other coil;
determining a certain voltage corresponding to a voltage across said other coil when said armature is approaching said core associated with said other coil; and
using said certain voltage as a feedback variable during said cycle to control energy to said other coil so as to control a velocity of said armature as said armature moves towards said core associated with said other coil.
an armature movable between first and second positions during a stroke of a cycle;
spring structure biasing said armature towards a resetting position generally between said first and second positions;
a stator having a coil and a core at said first position, said coil being constructed and arranged to apply a magnetic force, when energized, to the armature to cause the armature to move towards and land at said core and to maintain said armature at said core for a predetermined period;
circuit structure providing a certain voltage which corresponds to magnetic flux of a magnetic circuit created by said coil, core and said armature; and
control structure to control movement of said armature, wherein said control structure is constructed and arranged to determine said certain voltage when said armature is approaching said core, and to use said certain voltage as a feedback variable to control energy to said coil and thus control a velocity of said armature as said armature moves towards said core; characterised in that said circuit structure is constructed and arranged to provide a parametrically determined voltage which mirrors a terminal voltage of said coil, said control structure using said parametrically determined voltage as said feedback variable, said parametrically determined voltage defining said certain voltage.
das Leiten eines Signals mit Logikpegel über die besagte Pufferstufe, wobei die Schienenspannung an der besagten Pufferstufe von einer maßstäblich verkleinerten Kopie einer Hochspannungsversorgung des besagten Stellgliedes abgeleitet wird, und
das Glätten einer maßstäblich verkleinerten und gepufferten Pulsfolge von der besagten Pufferstufe mit dem besagten Tiefpassfilter, wobei ein Ausgang des besagten Tiefpassfilters die besagte parametrisch bestimmte Spannung definiert.
das selektive Erregen der anderen der besagten Spulen, um den besagten Anker mit einer gewissen Geschwindigkeit zu dem zu der besagten anderen Spule gehörigen Kern hin anzuziehen;
das Bestimmen einer gewissen Spannung, die einem Spannungsabfall an der besagten anderen Spule entspricht, wenn sich der besagte Anker dem besagten zu der besagten anderen Spule gehörigen Kern nähert; und
die Verwendung der besagten gewissen Spannung als Rückführgröße während des besagten Zyklus zur Steuerung der der besagten anderen Spule zugeführten Energie, um die Geschwindigkeit des besagten Ankers zu steuern, wenn sich der besagte Anker zu dem besagten zu der besagten anderen Spule gehörigen Kern hin bewegt.
einen Anker, der sich während eines Hubs eines Zyklus zwischen einer ersten und einer zweiten Position bewegen kann;
eine Federkonstruktion, die den besagten Anker in Richtung einer Rückstellposition vorbelastet, die sich im Wesentlichen zwischen der besagten ersten und der besagten zweiten Position befindet;
einen Ständer, der eine Spule und einen Kern in der besagten ersten Position aufweist, wobei die besagte Spule so konstruiert und angeordnet ist, dass sie, wenn sie erregt wird, eine magnetische Kraft auf den Anker ausübt, um zu bewirken, dass sich der Anker zu dem besagten Kern hin bewegt und an ihm zur Anlage kommt und dass der besagte Anker für eine vorgegebene Zeitdauer an dem besagten Kern gehalten wird;
eine Schaltungsanordnung, die eine gewisse Spannung zur Verfügung stellt, welche einem Magnetfluss eines von der besagten Spule, dem Kern und dem besagten Anker erzeugten Magnetkreises entspricht; und
eine Steuerungsanordnung, um die Bewegung des besagten Ankers zu steuern, wobei die besagte Steuerungsanordnung so konstruiert und gestaltet ist, dass sie die besagte gewisse Spannung bestimmt, wenn sich der besagte Anker dem besagten Kern nähert, und die besagte gewisse Spannung als eine Rückführgröße zur Steuerung der der besagten Spule zugeführten Energie verwendet und folglich die Geschwindigkeit des besagten Ankers steuert, wenn sich der besagte Anker zu dem besagten Kern hin bewegt; dadurch gekennzeichnet, dass die besagte Steuerungsanordnung so konstruiert und gestaltet ist, dass sie eine parametrisch bestimmte Spannung zur Verfügung stellt, welche eine Klemmenspannung der besagten Spule widerspiegelt, wobei die besagte Steuerungsanordnung die besagte parametrisch bestimmte Spannung als die besagte Rückführgröße verwendet, wobei die besagte parametrisch bestimmte Spannung die besagte gewisse Spannung definiert.
l'acheminement d'un signal de niveau logique provenant du régulateur de courant à travers ledit tampon, la tension de rail au niveau dudit tampon étant dérivée d'une réplique réduite d'une alimentation en haute tension dudit actionneur, et
le lissage d'un train d'impulsions mis à l'échelle et tamponné en provenance dudit tampon avec ledit filtre passe-bas, une sortie dudit filtre passe-bas définissant ladite tension déterminée de façon paramétrée.
l'excitation sélective de l'autre desdites bobines pour attirer l'induit à une certaine vitesse vers le noyau associé à ladite autre bobine ;
la détermination d'une certaine tension correspondant à une tension à travers ladite autre bobine quand ledit induit s'approche dudit noyau associé à ladite autre bobine ; et
l'utilisation de ladite certaine tension comme variable de réaction pendant ledit cycle pour commander l'énergie destinée à ladite autre bobine de façon à commander une vitesse dudit induit lorsque ledit induit se déplace vers ledit noyau associé à ladite autre bobine.
un induit mobile entre des première et deuxième positions pendant une course d'un cycle ;
une structure de ressort sollicitant ledit induit vers une position de réarmement généralement entre lesdites première et deuxième positions ;
un stator ayant une bobine et un noyau dans ladite première position, ladite bobine étant réalisée et agencée pour appliquer, quand elle est excitée, une force magnétique à l'induit pour amener l'induit à se déplacer vers ledit noyau et l'accoster et pour maintenir ledit induit au niveau dudit noyau pendant une période prédéfinie ;
une structure de circuit fournissant une certaine tension qui correspond aux flux magnétiques d'un circuit magnétique créé par ladite bobine, ledit noyau et ledit induit ; et
une structure de commande pour commander le mouvement dudit induit, où ladite structure de commande est réalisée et agencée pour déterminer ladite certaine tension quand ledit induit s'approche dudit noyau, et pour utiliser ladite certaine tension comme variable de réaction pour commander l'énergie destinée à ladite bobine et commander ainsi une vitesse dudit induit quand ledit induit se déplace vers ledit noyau ; caractérisé en ce que ladite structure de circuit est réalisée et agencée pour fournir une tension déterminée de façon paramétrée qui reflète une tension aux bornes de ladite bobine, ladite structure de commande utilisant ladite tension déterminée de façon paramétrée comme ladite variable de réaction, ladite tension déterminée de façon paramétrée définissant ladite certaine tension.